= {x ∈ l2| v(x) + c = 0}, where v: l2→ R, such that v(a) = v(π≤ma)and c∈ R.
Any convex and bounded subset U⊂ is called a local section.
Let WZ=a⊕ π>mWq,S, where ais an open convex subset of π≤ml2. Definition 36. A local section Z is said to be transversal in WZif
WZ∩ Z = Z, WZ= WZ,−∪ Z ∪ WZ,+, where
WZ,−= {x ∈ WZ| v(x) + c < 0}, WZ,+= {x ∈ WZ| v(x) + c > 0}, satisfying the condition
v (f (x))) >0, ∀x ∈ WZ. (A.4)
We will refer to (A.4) as the transversality condition.
We have the following easy lemma.
Lemma 37. Let Z be a local transversal section in WZfor (9) and let N⊂ Wq,Sfor some S > 0.
Assume that there exist t1, t2∈ R, t1< t2, such that the following conditions hold for all x∈ N:
ϕ((t1, t2), x)⊂ WZ, ϕ(t1, x)∈ WZ,− and ϕ(t2, x)∈ WZ,+.
Then, for each x0∈ N, there exists unique tZ(x0) ∈ (t1, t2), such that ϕ (tZ(x0), x0)∈ Z. Also, tZ: N → [t1, t2] is continuous.
Using the above lemma we can define a map PZ1→Z2 : Z1→ Z2 for two transversal local sections Z1and Z2, by
PZ1→Z2(x)= ϕ(tZ2(x), x).
A.4. Representation of h-sets and computer-assisted verification of covering relations with one exit direction
Algorithms for computer-assisted verification of covering relations for finite dimensional maps with arbitrary unstable dimension are presented in [42]. Although they can be directly extended to the case of infinite dimensional systems, for self-consistency of the article we pro-vide here a special case, when h-sets have one exit (nominally unstable) direction, i.e. u(N ) = 1 in Definition2.
Let us fix q > 1. In order to treat the system (8) rigorously on a computer we define a data structure which represents h-sets in l2,q:
type HSet where cNis an invertible affine map
cN
Since we assumed u(N ) = 1 in Definition2, the tail of N is always given by
TN= [−1, 1] ·
B =
=⇒ Nf 1reduces to a finite set of inequalities which must be satisfied. These are:
• πi(B) ⊂ (−1, 1) for i = 2, . . . , m,
• S(B) < S(N1), where S is a positive constant in h-set representation (A.5),
• either π1(Bl) <−1 and π1(Br) >1 or π1(Bl) >1 and π1(Br) <−1.
The two cases in the last condition depend on whether the mapping f changes or not the orien-tation along the exit direction. It is easy to see that
H (t,·) = (1 − t) whether f preserves or not the orientation in the exit direction.
A.5. Technical data
The source code of the C++11 program that realises the computer-assisted proof of Lemma10 is available at [38]. Below we list our choices of some parameters of the algorithms.
• All h-sets that appear in Lemma10are represented as a data structure (A.5) with the constant m = 15.
• We set d = 4 as the order of the Taylor method (Section4.4.3) for rigorous integration of (8).
• High-Order Enclosure (Section4.4.2) with d= 4 acts on m = 11 number of modes.
Verification of covering relation N0
=⇒ Nf 1 requires computation of three images of f — see (A.6). In Lemma10we verify 26 covering relations which means, that we have to check 78 = 3 · 26 inclusions.
We run the program which checks all the inequalities required for covering relations listed in Lemma10on a computer equipped with 64 physical cores (128 threads) Intel(R) Xeon(R) CPU E7-8867 v4 @ 2.40 GHz processors. The program finished after 40 minutes, which is the CPU time needed for the longest integration in N28→1=⇒ NP6 29→1.
The algorithm for rigorous integration of the KS equation is a part of the CAPD library [3].
We tested the program with CAPD version 5.0.59 and the C++11 compiler from gcc-5.2 suite.
References
[1]G.Arioli,H.Koch,Integrationofdissipativepartialdifferentialequations:acasestudy,SIAMJ.Appl.Dyn.Syst.
9(2010)1119–1133.
[2]G.Arioli,P.Zgliczy´nski,SymbolicdynamicsfortheHénon–HeilesHamiltonianonthecriticalenergylevel,J.
Differ.Equ.171(2001)173–202.
[3] CAPD- ComputerAssistedProofsinDynamics,apackageforrigorousnumerics,http://capd.ii.uj.edu.pl.
[4]P.Collet,J.-P.Eckmann,H.Epstein,J.Stubbe,AnalyticityfortheKuramoto–Sivashinskyequation,PhysicaD67 (1993)321–326.
[5]F.Christiansen,P.Cvitanovic,V.Putkaradze,Spatiotemporalchaosintermsofunstablerecurrentpatterns, Nonlin-earity10(1997)55–70.
[6]G.F.Corliss,R.Rihm,Validatinganapriorienclosureusinghigh-orderTaylorseries,in:G.Alefeld,A. From-mer(Eds.),ScientificComputing,ComputerArithmetics,andValidatedNumerics,AkademieVerlag,Berlin,1996, pp. 228–238.
[7]R.Easton,Isolatingblocksandsymbolicdynamics,J.Differ.Equ.17(1975)96–118.
[8]R.Easton,HomoclinicphenomenainHamiltoniansystemswithseveraldegreesoffreedom,J.Differ.Equ.29 (1978)241–252.
[9]M.J.Feigenbaum,Quantitativeuniversalityforaclassofnonlineartransformations,J.Stat.Phys.19(1978)25–52.
[10]J.Figueras,R.delaLlave,Numericalcomputationsandcomputerassistedproofsofperiodicorbitsofthe Kuramoto-Sivashinskyequation,SIAMJ.Appl.Dyn.Syst.16 (2)(2017)834–852.
[11]J.Figueras,M.Gameiro,J.P.Lessard,R.delaLlave,Aframeworkforthenumericalcomputationandaposteriori verificationofinvariantobjectsofevolutionequations,SIAMJ.Appl.Dyn.Syst.16 (2)(2017)1070–1088.
[12]C.Foias,B.Nicolaenko,G.Sell,R.Temam,InertialmanifoldsfortheKuramoto–Sivashinskyequationandan estimateoftheirlowestdimension,J.Math.PuresAppl.67(1988)197–226.
[13]C.Foias,R.Temam,GevreyclassregularityforthesolutionsoftheNavier-Stokesequations,J.Funct.Anal.87 (2) (1989)359–369.
[14]E.Hairer,S.P.Nørsett,G.Wanner,SolvingOrdinaryDifferentialEquationsI,NonstiffProblems,Springer-Verlag, Berlin, Heidelberg,1987.
[15]Z.Galias,P.Zgliczy´nski,ComputerassistedproofofchaosintheLorenzsystem,PhysicaD115(1998)165–188.
[16]M.Gameiro,J.-P.Lessard,Aposterioriverificationofinvariantobjectsofevolutionequations:periodicorbitsinthe Kuramoto-SivashinskyPDE,SIAMJ.Appl.Dyn.Syst.16 (1)(2017)687–728.
[17]A.Granas,J.Dugundji,FixedPointTheory,SpringerMonographsinMathematics,2010.
[18]A.Griewank,EvaluatingDerivatives:PrinciplesandTechniquesofAlgorithmicDifferentiation,Frontiersin Ap-pliedMathematics,vol. 19,SIAM,2000.
[19]J. Guckenheimer,P. Holmes, NonlinearOscillations, Dynamical Systems,and Bifurcations of VectorFields, SpringerVerlag,Berlin,Heidelberg,NewYork,1983.
[20]J.Hyman,B.Nicolaenko,TheKuramoto–Sivashinskyequation: abridgebetweenPDEsanddynamicalsystems, PhysicaD18(1986)113–126.
[21]M.E.Johnsohn,M.Jolly,I.Kevrekidis,TheOsebergtransition:visualizationoftheglobalbifurcationsforthe Kuramoto-Sivashinskyequation,Int.J.Bifurc.Chaos11(2001)1–18.
[22]M.Jolly,I.Kevrekidis,E.Titi,ApproximateinertialmanifoldsfortheKuramoto–Sivashinskyequation:analysis andcomputations,PhysicaD44(1990)38–60.
[23]Y.Kuramoto,T.Tsuzuki,Persistentpropagationofconcentrationwavesindissipativemediafarfromthermal equi-librium,Prog.Theor.Phys.55(1976)365.
[24]R.J.Lohner,Computationofguaranteedenclosuresforthesolutionsofordinaryinitialandboundaryvalue prob-lems,in:J.R.Cash,I.Gladwell(Eds.),ComputationalOrdinaryDifferentialEquations,ClarendonPress,Oxford, 1992.
[25]J.Mawhin,Leray-Schauderdegree:ahalfcenturyofextensionsandapplications,Topol.MethodsNonlinearAnal.
14(1999)105–228.
[26]R.E.Moore,MethodsandApplicationsofIntervalAnalysis,SIAM,Philadelphia,1979.
[27]K.Mischaikow,M.Mrozek,ChaosintheLorenzequations:acomputerassistedproof,Bull.Am.Meteorol.Soc.
32(1995)66–72.
[28]K.Mischaikow,M.Mrozek,Isolatingneighborhoodsandchaos,Jpn.J.Ind.Appl.Math.12(1995)205–236.
[29]J.Moser,StableandRandomMotionsinDynamicalSystems,PrincetonUniv.Press,1973.
[30]N.S.Nedialkov,K.R.Jackson,J.D.Pryce,Aneffectivehigh-orderintervalmethodforvalidatingexistenceand uniquenessofthesolutionofanIVPforanODE,Reliab.Comput.7 (6)(2001)449–465.
[31]B.Nicolaenko,B.Scheurer,R.Temam,SomeglobaldynamicalpropertiesoftheKuramoto-Sivashinskyequations:
nonlinearstabilityandattractors,PhysicaD16(1985)155–183.
[32]T.Rage,A.Neumaier,C.Schlier,Rigorousverificationofchaosinamolecularmodel,Phys.Rev.E50(1994) 2682–2688.
[33]G.I.Sivashinsky,Nonlinearanalysisofhydrodynamicalinstabilityinlaminarflames–1.Derivationofbasic equa-tions,ActaAstron.4 (11–12)(1977)1177–1206.
[34]Y.S.Smyrlis,D.T.Papageorgiou,Predicting chaosforinfinite-dimensionaldynamicalsystems:the Kuramoto-Sivashinskyequation,acasestudy,Proc.Natl.Acad.Sci.USA88 (24)(1991)11129–11132.
[35]R.Temam,Infinite-DimensionalDynamicalSystemsinMechanicsandPhysics,AppliedMathematicalSciences, vol. 68,Springer,1997.
[36]W.Tucker,Lorenzattractorexists,C.R.Acad.Sci.Paris,Ser.I328(1999)1197–1202.
[37]W.Tucker,ArigorousODEsolverandSmale’s14thproblem,Found.Comput.Math.2 (1)(2002)53–117.
[38] D.Wilczak,http://www.ii.uj.edu.pl/~{w}ilczak,personalhomepage.
[39]D.Wilczak,AbundanceofheteroclinicandhomoclinicorbitsforthehyperchaoticRösslersystem,DiscreteContin.
Dyn.Syst.,Ser.B11 (4)(2009)1039–1055.
[40]D.Wilczak,S.Serrano,R.Barrio,Coexistenceanddynamicalconnectionsbetweenhyperchaosandchaosinthe 4DRösslersystem:acomputer-assistedproof,SIAMJ.Appl.Dyn.Syst.15 (1)(2016)356–390.
[41]D.Wilczak,P.Zgliczy´nski,Heteroclinicconnectionsbetweenperiodicorbitsinplanarrestrictedcircularthreebody problem- acomputerassistedproof,Commun.Math.Phys.234 (1)(2003)37–75.
[42]D.Wilczak,P.Zgliczy´nski,Topologicalmethodforsymmetricperiodicorbitsformapswithareversingsymmetry, DiscreteContin.Dyn.Syst.,Ser.A17 (3)(2007)629–652.
[43] D.Wilczak,P.Zgliczy´nski,ArigorousC1-algorithmforintegrationofdissipativePDEsbasedonautomatic differ-entiationandtheTaylormethod,inpreparation.
[44]P.Zgliczy´nski,Fixedpointindexforiterationsofmaps,topologicalhorseshoeandchaos,Topol.MethodsNonlinear Anal.8(1996)169–177.
[45]P.Zgliczy´nski,Sharkovskii’stheoremformultidimensionalperturbationsofone-dimensionalmapsII,Topol. Meth-odsNonlinearAnal.14(1999)169–182.
[46]P.Zgliczy´nski,K.Mischaikow,Rigorousnumericsforpartialdifferentialequations:theKuramoto-Sivashinsky equation,Found.Comput.Math.1(2001)255–288.
[47]P.Zgliczy´nski,AttractingfixedpointsfortheKuramoto-Sivashinskyequation- acomputerassistedproof,SIAMJ.
Appl.Dyn.Syst.1(2002)215–235.
[48]P.Zgliczy´nski,TrappingregionsandanODE-typeproofofanexistenceanduniquenessforNavier-Stokesequations withperiodicboundaryconditionsontheplane,Univ.Iagel.ActaMath.41(2003)89–113.
[49]P.Zgliczy´nski,OnsmoothdependenceoninitialconditionsfordissipativePDEs,anODE-typeapproach,J.Differ.
Equ.195 (2)(2003)271–283.
[50]P.Zgliczy´nski,ComputerassistedproofofchaosintheRösslerequationsandintheHénonmap,Nonlinearity10 (1) (1997)243–252.
[51]P.Zgliczy´nski,RigorousnumericsfordissipativepartialdifferentialequationsII.Periodicorbitforthe Kuramoto-SivashinskyPDE- acomputerassistedproof,Found.Comput.Math.4(2004)157–185.
[52]P.Zgliczy´nski,M.Gidea,Coveringrelationsformultidimensionaldynamicalsystems,J.Differ.Equ.202 (1)(2004) 33–58.
[53]P.Zgliczy´nski,RigorousnumericsfordissipativePDEsIII.Aneffectivealgorithmforrigorousintegrationof dissi-pativePDEs,Topol.MethodsNonlinearAnal.36(2010)197–262.